Weak Interactions, Volume 71M. Baldo Ceolin, Società italiana di fisica |
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Page 214
... physical : y > 0 . This application of ve kinematics appears self - evident , but it is non- trivial because of the limited measuring accuracy , notably in angle , which causes losses of true events . For this reason , the first ...
... physical : y > 0 . This application of ve kinematics appears self - evident , but it is non- trivial because of the limited measuring accuracy , notably in angle , which causes losses of true events . For this reason , the first ...
Page 215
... physical region ( hatched ) is the hyperbola y = 0 , the other boundary is E 800 MeV . -- = There is a distinct concentration of events in the physical ve region ( fig . 17 ā ) ) . Points above y = 1 are surely background . Suppose the ...
... physical region ( hatched ) is the hyperbola y = 0 , the other boundary is E 800 MeV . -- = There is a distinct concentration of events in the physical ve region ( fig . 17 ā ) ) . Points above y = 1 are surely background . Suppose the ...
Page 364
... physical parameters of QCD ? Obviously the quark masses mur are free parameters , which must , at this stage , be intro- duced by hand from outside . They have nothing to do directly with the dynamics of QCD ; they play a role similar ...
... physical parameters of QCD ? Obviously the quark masses mur are free parameters , which must , at this stage , be intro- duced by hand from outside . They have nothing to do directly with the dynamics of QCD ; they play a role similar ...
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Common terms and phrases
algebra angle antineutrino Aµ(x background BJORKEN bosons branching ratio Cabibbo calculated CDHS CERN chamber charge charged-current charmed particles colour conservation coupling constant covariant covariant derivative cross-section decay modes define detector diagonal diagram dimuon events discussed distribution doublets electron energy equation experimental experiments FAISSNER fermions field flavour flux function Gargamelle gauge group gauge theories GeV/c gives GLASHOW gluons Goldstone hadron Higgs invariant isospin kaons Lagrangian lepton Lett mass matrix mass term massless MeV/c² momentum muon neutral currents neutral-current neutrino and antineutrino neutrino beam Nucl nucleon observed obtained orthogonal parameters parity violation parton Phys physical pion production proton Q₁ quark mass reactions Rendiconti S.I.F. representation scalar scattering sin² singlets spectrum strong interactions SU₂ symmetry target transformation U₁ vacuum expectation values vacuum vector weak WEINBERG y-distributions zero µ²